Let us review the well known IR behavior of the model [1]}, [2]}, [3]}. The non-anomalous continuous global symmetry group is \(SU(F)\times SU(F)\times U(1)_B\times U(1)_R\) . The gauge-invariant operators which describe the moduli space of the massless theory (at the classical level) are the mesons \(M_I^J=Q_I^{\alpha }\tilde{Q}^J_{\alpha }\) , the baryon \(B=\epsilon ^{I_1\dots I_{N}}\epsilon _{\alpha _{1}\dots \alpha _{N}}Q^{\alpha _1}_{I_1}\cdots Q^{\alpha _{N}}_{I_{N}}\)  and anti-baryon \(\tilde{B}=\epsilon _{I_1\dots I_{N}}\epsilon ^{\alpha _{1}\dots \alpha _{N}}\tilde{Q}_{\alpha _1}^{I_1}\cdots \tilde{Q}_{\alpha _{N}}^{I_{N}}\) .
The massless theory has classical moduli space which is singular at the origin when \(M_I^J=B=\widetilde{B}=0\) . However at the quantum mechanical level there is a constraint
\(\det M- B\tilde{B}=\Lambda ^{2N}.\) 
